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Neutron reflectometry Helmut Fritzsche NRC-SIMS, Canadian Neutron Beam Centre, Chalk River, Canada
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Canadian Neutron Beam Centre Outlook Application/advantages of neutron reflectometry Theoretical background Instrumental setup Experiments: Photoactive azobenzene films Hydrogen storage in MgAl films Element-specific hysteresis curves in ErFe 2 / DyFe 2 multilayers Supermirrors (non-polarizing and polarizing)
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Canadian Neutron Beam Centre What can be measured with neutron reflectometry? Film thickness (2 – 200 nm): swelling of polymer films due to water uptake film expansion during illumination of photoactive films film expansion during hydrogen absorption growth of oxide layer In-plane structures on nm and m scale Scattering length density profile: profile of absorbed gas/liquid interdiffusion magnetic structures magnetic field penetration into superconductors
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Canadian Neutron Beam Centre Specific advantages of neutron reflectometry Large penetration depth (for most materials): Buried layers In-situ measurements (cryostats, cryomagnets, high-pressure cells, furnaces) Spin and non-spin flip reflectivity: Magnetization reversal, magnetic structure No diamagnetic background of substrate for ferromagnetic samples: Determination of absolute magnetic moment High sensitivity to hydrogen: Determine hydrogen profile in hydrogen storage materials Change of contrast by using isotopes: swelling of films during water (vapor or liquid) uptake (H 2 O / D 2 O) expansion of films during hydrogen absorption (H 2 / D 2 )
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Canadian Neutron Beam Centre Reflection and refraction specularly reflected refracted incoming wave Physical origin: different index of refraction for two media medium 1: n 1 medium 2: n 2 Refraction: Snell‘s law n 1 sin 1 = n 2 sin 2 2 1 Reflection: r = 1 r
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Canadian Neutron Beam Centre Reflection and refraction: the critical angle reflected refracted medium 1: n 1 medium 2: n 2 90° c Critical angle: n 1 sin 1 = n 2 sin 90° sin c = n 2 / n 1 For 1 > c : no refracted beam exists, only a reflected beam Total reflection (100% reflectivity) occurs in the medium with the larger n
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Canadian Neutron Beam Centre Index of refraction for light For light with = 656 nm: Materialn c (for n 2 =1) Vacuum1.00- Water1.3348.8 Quartz glass1.4643.2 Benzene1.5041.8 What is the index of refraction for neutrons? Note: the index of refraction depends on the wavelength
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Canadian Neutron Beam Centre Index of refraction for neutrons z EzEz } E kin,1 V SLD E kin,2 Fermi’s pseudopotential: m: neutron mass : neutron wavelength b: nuclear scattering length : density of atoms b: scattering length density (SLD)
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Canadian Neutron Beam Centre Scattering lengths X-rays X-rays: b Z (electron density) Neutrons Neutrons: no systematics Important: not absolute number but contrast of SL X-rays and neutrons are complementary probes
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Canadian Neutron Beam Centre Index of refraction for neutrons: some examples For neutrons with = 0.237 nm: Materialn b (10 -4 1/nm 2 ) Vacuum 1.000 Water (H 2 O)1.000001-0.561 Si0.9999982.073 Quartz glass0.9999974.185 Heavy water (D 2 O)0.9999946.366 58 Ni 0.99998813.16 Note: n 1-10 -5 The deviation of n neutron from 1 is much smaller than for light, because the interaction of neutrons with matter is much weaker
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Canadian Neutron Beam Centre Reflectometry setup on D3 S1 S2 S3 S4 sample PG filter analyzer detector Focusing PG monochromator Polarizing supermirror Spin-down neutrons spin flipper
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Canadian Neutron Beam Centre Reflectometry setup on D3 S1 S2 S3 S4 sample PG filter analyzer detector Focusing PG monochromator Polarizing supermirror Spin-down neutrons spin flipper Spin-up neutrons
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Canadian Neutron Beam Centre The reflectometry experiment detector sample slit system q 22 q: scattering vector : scattering angle geometry: sample moves by detector moves by 2
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Canadian Neutron Beam Centre The reflectometry experiment detector sample slit system q Reflectometry: Measuring the reflected intensity as a function of q
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Canadian Neutron Beam Centre Visualization of a reflectivity curve (Si wafer) z EzEz reflectivity q } qcqc Si: c =0.11º (for =2.37 Å) 58 Ni: c =0.28º (for =2.37 Å)
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Canadian Neutron Beam Centre Kiessig fringes Oscillations due to total film thickness q 1/d q=2 /d qcqc
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Canadian Neutron Beam Centre Multilayer Bragg peaks bilayer Bragg peaks at q=2 /t q = n · 2 /62.8 Å -1 = n · 0.1 Å -1 Short period oscillations: Kiessig fringes Fe SLD Cr Fe Cr Si wafer Fe Cr } Bilayer thickness t t = 32.8 Å + 30 Å = 62.8 Å In total: 20 repetitions
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Canadian Neutron Beam Centre Magnetic interaction H ext : external magnetic field B : magnetic induction µ : magnetic moment of neutrons
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Canadian Neutron Beam Centre PNR: bulk Fe Different reflectivity for spin-up and spin-down neutrons Determination of the absolute magnetic moment possible qc-qc- qc+qc+ V nuc V spin up (R + )spin down (R - ) V nuc
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Canadian Neutron Beam Centre PNR: Fe/Cr multilayers Structural peak AF peak Ferromagnetic coupling: Magnetic period = chemical period Antiferromagnetic coupling: Magnetic period = 2 x chemical period
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Canadian Neutron Beam Centre In-situ setup for photoactive films lenses shuttermirror Neutron reflectometry and Laser illumination at the same time
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Canadian Neutron Beam Centre Results for azobenzene films 0.0 h 0.4 h 2.5 h 8.0 h Laser irradiation time Smaller q larger film thickness
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Canadian Neutron Beam Centre Co-sputtering of MgAl alloy films Mg Al Pd Vacuum Chamber Si Wafer
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Canadian Neutron Beam Centre Hydrogen absorption Hydrogen gas cylinder Absorption cell for thin films on wafers with up to 100 mm diameter
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Canadian Neutron Beam Centre Hydrogen desorption equipment Reflectometry furnace: Ar atmosphere or vacuum 300 K < T < 670 K sample heater thermocouple
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Canadian Neutron Beam Centre Mg 0.6 Al 0.4 at 298 K Mg 0.6 Al 0.4 Pd SiO 2 Si Fit: Pd: t = 104 Å = 4.4 Å MgAl: t = 520 Å = 15.7 Å
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Canadian Neutron Beam Centre Absorption in Mg 0.6 Al 0.4 increase of film thickness by about 20% hydrogen content is 83 at.% = 3.2 weight % SLD b H < 0 t t
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Canadian Neutron Beam Centre Annealing of a desorbed Mg 0.7 Al 0.3 film Pd layer does not exist anymore after 9 h: Pd diffuses into the MgAl layer
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Canadian Neutron Beam Centre DyFe 2 / ErFe 2 multilayer: element-specific hysteresis Magnetization reversal at 100 K After saturation at µ 0 H = –6 T (6 nm DyFe 2 / 6 nm ErFe 2 ) 40 ErFe 2 and DyFe 2 magnetizations are not parallel DyFe 2 : easy-axis loop ErFe 2 : hard-axis loop
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Canadian Neutron Beam Centre PNR is element-specific ErFe 2 DyFe 2 R + = R - nonmagnetic layers
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Canadian Neutron Beam Centre PNR is element-specific ErFe 2 DyFe 2 ErFe 2 DyFe 2 R + = R - ~R + ~R - nonmagnetic layers
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Canadian Neutron Beam Centre PNR is element-specific ErFe 2 DyFe 2 ErFe 2 DyFe 2 R + = R - ~R + ~R - nonmagnetic layers
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Canadian Neutron Beam Centre PNR is element-specific ErFe 2 DyFe 2 R + = R - ErFe 2 DyFe 2 ~R - ~R + ErFe 2 DyFe 2 ~R + ~R - nonmagnetic layers
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Canadian Neutron Beam Centre PNR is element-specific ErFe 2 DyFe 2 ErFe 2 DyFe 2 R + = R - ~R + ~R - ErFe 2 DyFe 2 ~R - ~R + nonmagnetic layers
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Canadian Neutron Beam Centre supermirror goal: Extend the range of neutron reflection beyond the regime of total reflection concept: continuous Bragg reflection from a multilayer composed of bilayers with a variation of the thickness realization: Ni/Ti multilayer, b Ni = 10.3 fm, b Ti = -3.4 fm 100 bilayers, q c = 2 x q c, Ni
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Canadian Neutron Beam Centre supermirror m-value: m = q c / q c, Ni Ni SLD Ni Ti Ni z
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Canadian Neutron Beam Centre Polarizing supermirror concept: Using the supermirror concept with a magnetic/non-magnetic bilayer The SLD of the bilayer is index-matched for spin-down neutrons no multilayer Bragg peaks for down-neutrons Spin-up neutrons show supermirror behavior with extended critical edge Fe/Co SLD spin-up neutrons Si Fe/Co Si spin-down neutrons Fe/Co SLD Si Fe/Co Si Index matching
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Canadian Neutron Beam Centre Polarizing supermirror: Fe-Co/Si Reflected intensity Transmitted intensity
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Canadian Neutron Beam Centre Flipping ratio Flipping ratio = usable range 25
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